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SOLAR PARABOLIC TROUGH 5-24 Figure 1. Solar/Rankine parabolic trough system schematic [1]. 1.0 System Description Parabolic trough technology is currently the most proven solar thermal electric technology. This is primarily due to nine large commercial-scale solar power plants, the first of which has been operating in the California Mojave Desert since 1984. These plants, which continue to operate on a daily basis, range in size from 14 to 80 MW and represent a total of 354 MW of installed electric generating capacity. Large fields of parabolic trough collectors supply the thermal energy used to produce steam for a Rankine steam turbine/generator cycle. Plant Overview Figure 1 shows a process flow diagram that is representative of the majority of parabolic trough solar power plants in operation today. The collector field consists of a large field of single-axis tracking parabolic trough solar collectors. The solar field is modular in nature and is composed of many parallel rows of solar collectors aligned on a north-south horizontal axis. Each solar collector has a linear parabolic-shaped reflector that focuses the sun’s direct beam radiation on a linear receiver located at the focus of the parabola. The collectors track the sun from east to west during the day to ensure that the sun is continuously focused on the linear receiver. A heat transfer fluid (HTF) is heated as it circulates through the receiver and returns to a series of heat exchangers in the power block where the fluid is used to

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Page 1: Solar Parabolic Trough - Ningapi.ning.com/.../solar_trough.pdfThe collector field consists of a large field of single-axis tracking parabolic trough solar collectors . The solar field

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Figure 1. Solar/Rankine parabolic trough system schematic [1].

1.0 System Description

Parabolic trough technology is currently the most proven solar thermal electric technology. This is primarily due tonine large commercial-scale solar power plants, the first of which has been operating in the California Mojave Desertsince 1984. These plants, which continue to operate on a daily basis, range in size from 14 to 80 MW and representa total of 354 MW of installed electric generating capacity. Large fields of parabolic trough collectors supply thethermal energy used to produce steam for a Rankine steam turbine/generator cycle.

Plant Overview

Figure 1 shows a process flow diagram that is representative of the majority of parabolic trough solar power plants inoperation today. The collector field consists of a large field of single-axis tracking parabolic trough solar collectors.The solar field is modular in nature and is composed of many parallel rows of solar collectors aligned on a north-southhorizontal axis. Each solar collector has a linear parabolic-shaped reflector that focuses the sun’s direct beam radiationon a linear receiver located at the focus of the parabola. The collectors track the sun from east to west during the dayto ensure that the sun is continuously focused on the linear receiver. A heat transfer fluid (HTF) is heated as itcirculates through the receiver and returns to a series of heat exchangers in the power block where the fluid is used to

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Figure 2. Integrated Solar Combined Cycle System [1].

generate high-pressure superheated steam. The superheated steam is then fed to a conventional reheat steamturbine/generator to produce electricity. The spent steam from the turbine is condensed in a standard condenser andreturned to the heat exchangers via condensate and feedwater pumps to be transformed back into steam. Condensercooling is provided by mechanical draft wet cooling towers. After passing through the HTF side of the solar heatexchangers, the cooled HTF is recirculated through the solar field.

Historically, parabolic trough plants have been designed to use solar energy as the primary energy source to produceelectricity. The plants can operate at full rated power using solar energy alone given sufficient solar input. Duringsummer months, the plants typically operate for 10 to 12 hours a day at full-rated electric output. However, to date,all plants have been hybrid solar/fossil plants; this means they have a backup fossil-fired capability that can be usedto supplement the solar output during periods of low solar radiation. In the system shown in Figure 1, the optionalnatural-gas-fired HTF heater situated in parallel with the solar field, or the optional gas steam boiler/reheater locatedin parallel with the solar heat exchangers, provide this capability. The fossil backup can be used to produce ratedelectric output during overcast or nighttime periods. Figure 1 also shows that thermal storage is a potential option thatcan be added to provide dispatchability.

Integrated Solar Combined Cycle System (ISCCS)

The ISCCS is a new design concept that integrates a parabolic trough plant with a gas turbine combined-cycleplant [2,3]. The ISCCS has generated much interest because it offers an innovative way to reduce cost and improvethe overall solar-to-electric efficiency. A process flow diagram for an ISCCS is shown in Figure 2. The ISCCS usessolar heat to supplement the waste heat from the gas turbine in order to augment power generation in the steam Rankinebottoming cycle. In this design, solar energy is generally used to generate additional steam and the gas turbine wasteheat is used for preheat and steam superheating. Most designs have looked at increasing the steam turbine size by asmuch as 100%. The ISCCS design will likely be preferred over the solar Rankine plant in regions where combinedcycle plants are already being built.

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Coal Hybrids

In regions with good solar resources where coal plants are currently used, parabolic trough plants can be integrated intothe coal plant to either reduce coal consumption or add solar peaking, much like the ISCCS configuration. Due to thehigher temperature and pressure steam conditions used in modern coal plants, the solar steam may need to be admittedin the intermediate or low-pressure turbine.

History

Organized, large-scale development of solar collectors began in the U.S. in the mid-1970s under the Energy Researchand Development Administration (ERDA) and continued with the establishment of the U.S. Department of Energy(DOE) in 1978. Parabolic trough collectors capable of generating temperatures greater than 500ºC (932ºF) wereinitially developed for industrial process heat (IPH) applications. Much of the early development was conducted byor sponsored through Sandia National Laboratories in Albuquerque, New Mexico. Numerous process heatapplications, ranging in size from a few hundred to about 5000 m of collector area, were put into service. Acurex,2

SunTec, and Solar Kinetics were the key parabolic trough manufacturers in the United States during this period.

Parabolic trough development was also taking place in Europe and culminated with the construction of the IEA SmallSolar Power Systems Project/Distributed Collector System (SSPS/DCS) in Tabernas, Spain, in 1981. This facilityconsisted of two parabolic trough solar fields with a total mirror aperture area of 7602 m . The fields used the single-2

axis tracking Acurex collectors and the double-axis tracking parabolic trough collectors developed by M.A.N. ofMunich, Germany. In 1982, Luz International Limited (Luz) developed a parabolic trough collector for IPHapplications that was based largely on the experience that had been gained by DOE/Sandia and the SSPS projects.

Although several parabolic trough developers sold IPH systems in the 1970s and 1980's, they generally found twobarriers to successful marketing of their technologies. First, there was a relatively high marketing and engineeringeffort required for even small projects. Second, most potential industrial customers had cumbersome decision-makingprocesses which often resulted in a negative decision after considerable effort had already been expended.

In 1983, Southern California Edison (SCE) signed an agreement with Acurex Corporation to purchase power from asolar electric parabolic trough power plant. Acurex was unable to raise financing for the project. Consequently, Luznegotiated similar power purchase agreements with SCE for the Solar Electric Generating System (SEGS) I and IIplants. Later, with the advent of the California Standard Offer (SO) power purchase contracts for qualifying facilitiesunder the Public Utility Regulatory Policies Act (PURPA), Luz was able to sign a number of SO contracts with SCEthat led to the development of the SEGS III through SEGS IX projects. Initially, the plants were limited by PURPAto 30 MW in size; later this limit was raised to 80 MW. Table 1 shows the characteristics of the nine SEGS plants builtby Luz.

In 1991, Luz filed for bankruptcy when it was unable to secure construction financing for its tenth plant (SEGS X).Though many factors contributed to the demise of Luz, the basic problem was that the cost of the technology was toohigh to compete in the power market. Lotker [5] describes the events that enabled Luz to successfully compete in thepower market between 1984 and 1990 and many of the institutional barriers that contributed to their eventual downfall.It is important to note that all of the SEGS plants were sold to investor groups as independent power projects andcontinue to operate today.

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Table 1. Characteristics of SEGS I through IX [4].

SEGS 1st Year of Net Solar Field Solar Field Solar Fossil AnnualPlant Operation Output Outlet Temp. Area Turbine Turbine Output

(MW ) (ºC/ºF) (m ) Eff. (%) Eff. (%) (MWh)e2

I 1985 13.8 307/585 82,960 31.5 - 30,100II 1986 30 316/601 190,338 29.4 37.3 80,500III & IV 1987 30 349/660 230,300 30.6 37.4 92,780V 1988 30 349/660 250,500 30.6 37.4 91,820VI 1989 30 390/734 188,000 37.5 39.5 90,850VII 1989 30 390/734 194,280 37.5 39.5 92,646VIII 1990 80 390/734 464,340 37.6 37.6 252,750IX 1991 80 390/734 483,960 37.6 37.6 256,125

Collector Technology

The basic component of the solar field is the solar collector assembly (SCA). Each SCA is an independently trackingparabolic trough solar collector made up of parabolic reflectors (mirrors), the metal support structure, the receiver tubes,and the tracking system that includes the drive, sensors, and controls. Table 2 shows the design characteristics of theAcurex, single axis tracking M.A.N., and three generations of Luz SCAs. The general trend was to build largercollectors with higher concentration ratios (collector aperture divided by receiver diameter) to maintain collectorthermal efficiency at higher fluid outlet temperatures.

Table 2. Solar collector characteristics [4,6].

Collector 3001 M480 LS-1 LS-2 LS-3Acurex M.A.N. Luz Luz Luz

Year 1981 1984 1984 1985 1988 1989

Area (m ) 34 80 128 235 5452

Aperture (m) 1.8 2.4 2.5 5 5.7

Length (m) 20 38 50 48 99

Receiver Diameter (m) 0.051 0.058 0.042 0.07 0.07

Concentration Ratio 36:1 41:1 61:1 71:1 82:1

Optical Efficiency 0.77 0.77 0.734 0.737 0.764 0.8

Receiver Absorptivity 0.96 0.96 0.94 0.94 0.99 0.96

Mirror Reflectivity 0.93 0.93 0.94 0.94 0.94 0.94

Receiver Emittance 0.27 0.17 0.3 0.24 0.19 0.19

@ Temperature (ºC/ºF) 300/572 300/572 350/662 350/662

Operating Temp. (ºC/ºF) 295/563 307/585 307/585 349/660 390/734 390/734

Luz System Three (LS-3) SCA: The LS-3 collector was the last collector design produced by Luz and was usedprimarily at the larger 80 MW plants. The LS-3 collector represents the current state-of-the-art in parabolic troughcollector design and is the collector that would likely be used in the next parabolic trough plant built. A more detaileddescription of the LS-3 collector and its components follows.

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LocalController

DrivePylon

IntermediatePylon

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Figure 3. Luz System Three Solar Collector Assembly (LS-3 SCA) [1].

Figure 3 shows a diagram of the LS-3 collector. The LS-3 reflectors are made from hot-formed mirrored glass panels,supported by the truss system that gives the SCA its structural integrity. The aperture or width of the parabolicreflectors is 5.76 m and the overall SCA length is 95.2 m (net glass). The mirrors are made from a low iron float glasswith a transmissivity of 98% that is silvered on the back and then covered with several protective coatings. The mirrorsare heated on accurate parabolic molds in special ovens to obtain the parabolic shape. Ceramic pads used for mountingthe mirrors to the collector structure are attached with a special adhesive. The high mirror quality allows 97% of thereflected rays to be incident on the linear receiver.

The linear receiver, also referred to as a heat collection element (HCE), is one of the primary reasons for the highefficiency of the Luz parabolic trough collector design. The HCE consists of a 70 mm steel tube with a cermet selectivesurface, surrounded by an evacuated glass tube. The HCE incorporates glass-to-metal seals and metal bellows toachieve the vacuum-tight enclosure. The vacuum enclosure serves primarily to protect the selective surface and toreduce heat losses at the high operating temperatures. The vacuum in the HCE is maintained at about 0.0001 mm Hg(0.013 Pa). The cermet coating is sputtered onto the steel tube to give it excellent selective heat transfer properties withan absorptivity of 0.96 for direct beam solar radiation, and a design emissivity of 0.19 at 350ºC (662ºF). The outerglass cylinder has anti-reflective coating on both surfaces to reduce reflective losses off the glass tube. Getters, metallicsubstances that are designed to absorb gas molecules, are installed in the vacuum space to absorb hydrogen and othergases that permeate into the vacuum annulus over time.

The SCAs rotate around the horizontal north/south axis to track the sun as it moves through the sky during the day. Theaxis of rotation is located at the collector center of mass to minimize the required tracking power. The drive systemuses hydraulic rams to position the collector. A closed loop tracking system relies on a sun sensor for the precisealignment required to focus the sun on the HCE during operation to within +/- 0.1 degrees. The tracking is controlledby a local controller on each SCA. The local controller also monitors the HTF temperature and reports operationalstatus, alarms, and diagnostics to the main solar field control computer in the control room. The SCA is designed fornormal operation in winds up to 25 mph (40 km/h) and somewhat reduced accuracy in winds up to 35 mph (56 km/h).The SCAs are designed to withstand a maximum of 70 mph (113 km/h) winds in their stowed position (the collectoraimed 30º below eastern horizon).

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The SCA structure on earlier generations of Luz collectors was designed to high tolerances and erected in place in orderto obtain the required optical performance. The LS-3 structure is a central truss that is built up in a jig and alignedprecisely before being lifted into place for final assembly. The result is a structure that is both stronger and lighter.The truss is a pair of V-trusses connected by an endplate. Mirror support arms are attached to the V-trusses.

Availability of Luz Collector Technology: Although no new parabolic trough plants have been built since 1991, spareparts for the existing plants are being supplied by the original suppliers or new vendors. The two most critical andunique parts are the parabolic mirrors and the HCEs. The mirrors are being provided by Pilkington Solar International(PilkSolar) and are manufactured on the original SEGS mirror production line. The Luz HCE receiver tubemanufacturing facility and technology rights were sold to SOLEL Solar Systems Ltd. of Jerusalem, Israel. SOLELcurrently supplies HCEs as spare parts for the existing SEGS plants. Should a commercial opportunity arise, it is likelythat a consortium of participants would form to supply Luz parabolic trough collector technology.

SEGS Plant Operating Experience

The nine operating SEGS plants have demonstrated the commercial nature of the Luz parabolic trough collectortechnology and have validated many of the SEGS plant design concepts. Additionally, many important lessons havebeen learned related to the design, manufacture, construction, operation, and maintenance of large-scale parabolictrough plants [7,8,9].

Solar Field Components: A simple problem with a single component, such as an HCE, can affect many thousands ofcomponents in a large solar field. Thus it is essential that each of the SCA components is designed for the 30-year lifeof the plant and that a sufficient QA/QC program is in place to ensure that manufacture and installation adhere todesign specifications. Luz used three generations of collector during the development of the nine SEGS plants. Eachtime a new generation of collector was used, some form of component failure was experienced. However, one of themajor achievements of Luz was the speed with which they were able to respond to new problems as they wereidentified. Problems with components were due to design or installation flaws. An important lesson from the plantshas been the recognition that O&M requirements need to be fully integrated into the design. Three components inparticular are worthy of discussion because they have represented the largest problems experienced: HCEs, mirrors,and flexhoses.

Heat Collection Elements (HCEs): A number of HCE failure mechanisms have been identified at the SEGS plants, withall of these issues resolved through the development of improved installation practices and operation procedures, orthrough a design modification. Loss of vacuum, breakage of the glass envelope, deterioration of the selective surface,and bowing of the stainless steel tube (which eventually can lead to glass breakage) have been the primary HCEfailures, all of which affect thermal efficiency. Several of the existing SEGS plants have experienced unacceptablyhigh HCE glass envelope breakage rates. The subsequent exposure to air accelerates degradation of the selectivesurface. Design improvements have been identified to improve durability and performance, and these have beenintroduced into replacement parts manufactured for the existing plants. In addition, better installation and operationalprocedures have significantly reduced HCE failures. Future HCE designs should: (1) use new tube materials tominimize bowing problems; (2) allow broken glass to be replaced in-situ in the field; and (3) continue to improve theselective coating absorptance, emittance, and long-term stability in air.

Mirrors: The current low iron glass mirrors are one of the most reliable components in the Luz collectors. Separationof the mirror mounting pads from the mirrors was an early problem caused by differential thermal expansion betweenthe mirror and the pad. This problem was resolved by using ceramic pads, a more pliable adhesive, and thermalshielding. In addition, methods have been developed that allow the O&M crew to retrofit the older mirror pad designand strengthen them to greatly reduce failures. Mirror breakage due to high winds has been observed near the edges

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of the solar field where wind forces can be high. Strengthened glass mirrors or thin plastic silvered film reflectors havebeen designed to circumvent this problem. In general, there has been no long-term degradation in the reflective qualityof the mirrors; ten year old mirrors can be cleaned and brought back to like-new reflectivity. However, the glassmirrors are expensive and for the cost of the collector to be reduced, alternative mirrors are necessary. Any new mirrormust be able to be washed without damaging the optical quality of the mirror. Front surface mirrors hold potential tohave higher reflectivity, if the long-term performance and washability can be demonstrated.

Flexhoses: The flexhoses that connect the SCAs to the headers and SCAs to each other have experienced high failurerates at the early SEGS plants. Later plants used an improved design with a substantially increased life thatsignificantly reduced failures. In addition, a new design that replaces the flexhoses with a hard piped assembly withball joints is being used at the SEGS III-VII plants located at Kramer Junction. The new ball joint assembly has anumber of advantages over flexhoses including lower cost, a significant reduction in pressure drop, and reduced heatlosses. If ball joint assemblies can be proven to have a life comparable to the new longer-life flexhoses, then they willbe included in all future trough designs.

Mirror Washing & Reflectivity Monitoring: Development of an efficient and cost-effective program for monitoringmirror reflectivity and washing mirrors is critical. Differing seasonal soiling rates require flexible procedures. Forexample, high soiling rates of 0.5%/day have been experienced during summer periods. After considerable experience,O&M procedures have settled on several methods, including deluge washing, and direct and pulsating high-pressuresprays. All methods use demineralized water for good effectiveness. The periodic monitoring of mirror reflectivitycan provide a valuable quality control tool for mirror washing and help optimize wash labor. As a general rule, thereflectivity of glass mirrors can be returned to design levels with good washing.

Maintenance Tracking: In recent years, computerized maintenance management software (CMMS) has found wideacceptance for use in conventional fossil power plant facilities. CMMS systems can greatly enhance the planning andefficiency with which maintenance activities are carried out, reduce maintenance costs, and often result in improvedavailability of the power plant. CMMS programs have been implemented at trough power plants as well, but thesoftware is not ideally suited for the solar field portion of the plant. CMMS systems excel in applications that havea thousand unique pieces of equipment, but are not really suited to handle systems with a thousand of the same kindof equipment, like SCAs in a solar field. For this reason, custom database programs have been developed to trackproblems and schedule maintenance in the solar plant. These programs have proven to be an essential tool for trackingand planning solar field maintenance activities and should be considered to be essential for any new project.

Collector Alignment: Operational experience has shown that it is important to be able to periodically check collectoralignment and to be able to correct alignment problems when necessary. Collector designs should allow field alignmentchecks and easy alignment corrections.

Project Start-up Support: Operation of a solar power plant differs from conventional fossil-fuel power plant operationin several ways, primarily due to the solar field equipment and operations requirements, integration of the solar fieldwith the power block, and the effects of cyclic operation. Much knowledge has been gained from the existing SEGSplants that is applicable to the development of procedures, training of personnel, and the establishment of an effectiveO&M organization.

Thermal Cycling and Daily Startup: Typically, parabolic trough plants are operated whenever sufficient solar radiationexists, and the backup fossil is only used to fill in during the highest value non-solar periods. As a result, the plantsare typically shut down during the night and restarted each morning. The plants must be designed to not only be startedon a daily basis, but also to start up as quickly as possible. Since the current SEGS plant design does not includethermal storage, the solar field and power block are directly coupled. The use of thermal storage can significantly

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1988 1989 1990 1991 1992 1993 1994 1995 199696

98

100

102

104

106

108

110

112SEGS IIISEGS IVSEGS VSEGS VISEGS VII

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Figure 4. On-peak capacity factors for five 30 MW SEGS plants during 1988 to 1996 [10].

mitigate these problems. In general, equipment/system design specifications and operating procedures must bedeveloped with these requirements in mind. Both normal engineering considerations and the experience from theSEGS plants provide important inputs into these needs. Mundane design features such as valves, gaskets, and sealsand bolt selection can be an expensive problem unless properly specified.

2.0 System Application, Benefits, and Impacts

Large-scale Grid Connected Power: The primary application for parabolic trough power plants is large-scale gridconnected power applications in the 30 to 300 MW range. Because the technology can be easily hybridized with fossilfuels, the plants can be designed to provide firm peaking to intermediate load power. The plants are typically a goodmatch for applications in the U.S. southwest where the solar radiation resource correlates closely with peak electricpower demands in the region. The existing SEGS plants have been operated very successfully in this fashion to meetSCE’s summer on-peak time-of-use rate period. Figure 4 shows the on-peak performance of the SEGS III throughSEGS VII plants that are operated by KJC Operating Company. The chart shows that all 5 plants have producedgreater than 100% of their rated capacity during the critical on-peak period between 1200 and 1800 PDT on weekdaysduring June through September. This demonstrates the continuous high availability these plants have been able toachieve. Note that 1989 was the first year of operation for SEGS VI and SEGS VII.

Domestic Market: The primary domestic market opportunity for parabolic trough plants is in the Southwestern desertswhere the best direct normal solar resources exist. These regions also have peak power demands that could benefitfrom parabolic trough technologies. In particular, California, Arizona, and Nevada appear to offer some of the bestopportunities for new parabolic trough plant development. However, other nearby states may provide excellentopportunities as well. The current excess of electric generating capacity in this region and the availability of low costnatural gas make future sustained deployment of parabolic trough technology in this region unlikely unless other factorscome into play. However, with utility restructuring, and an increased focus on global warming and other environmentalissues, many new opportunities such as renewable portfolio standards and the development of solar enterprise zonesmay encourage the development of new trough plants. All of the existing Luz-developed SEGS projects weredeveloped as independent power projects and were enabled through special tax incentives and power purchaseagreements such as the California SO-2 and SO-4 contracts.

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International Markets: With the high demand for new power generation in many developing countries, the nextdeployment of parabolic troughs could be abroad. Many arid regions in developing countries are ideally suited forparabolic trough technologies. India, Egypt, Morocco, Mexico, Brazil, Crete (Greece), and Tibet (China) haveexpressed interest in trough technology power plants. Many of these countries are already planning installations ofcombined cycle projects. For these countries, the trough ISCCS design may provide a cheap and low risk opportunityto begin developing parabolic trough power plants. In regions such as Brazil and Tibet that have good direct normalsolar resources and existing large hydroelectric and/or pumped storage generation resources, parabolic troughtechnologies can round out their renewable power portfolio by providing additional generation during the dry season.

Benefits

Least Cost Solar Generated Electricity: Trough plants currently provide the lowest cost source of solar generatedelectricity available. They are backed by considerable valuable operating experience. Troughs will likely continue tobe the least-cost solar option for another 5-10 years depending on the rate of development and acceptance of other solartechnologies.

Daytime Peaking Power: Parabolic trough power plants have a proven track record for providing firm renewabledaytime peaking generation. Trough plants generate their peak output during sunny periods when air conditioningloads are at their peak. Integrated natural gas hybridization and thermal storage have allowed the plants to provide firmpower even during non-solar and cloudy periods.

Environmental: Trough plants reduce operation of higher-cost, cycling fossil generation that would be needed to meetpeak power demands during sunny afternoons at times when the most photochemical smog, which is aggravated byNO emissions from power plants, is produced.X

Economic: The construction and operation of trough plants typically have a positive impact on the local economy. Alarge portion of material during construction can generally be supplied locally. Also trough plants tend to be fairlylabor-intensive during both construction and operation, and much of this labor can generally be drawn from local labormarkets.

Impacts

HTF Spills/Leaks: The current heat transfer fluid (Monsanto Therminol VP-1) is an aromatic hydrocarbon,biphenyl-diphenyl oxide. The oil is classified as non-hazardous by U.S. standards but is a hazardous material in thestate of California. When spills occur, contaminated soil is removed to an on-site bio-remediation facility that utilizesindigenous bacteria in the soil to decompose the oil until the HTF concentrations have been reduced to acceptablelevels. In addition to liquid spills, there is some level of HTF vapor emissions from valve packing and pump sealsduring normal operation [11]. Although the scent of these vapor emissions is often evident, the emissions are wellwithin permissible levels.

Water: Water availability can be a significant issue in the arid regions best suited for trough plants. The majority ofwater consumption at the SEGS plants (approximately 90%) is used by the cooling towers. Water consumption isnominally the same as it would be for any Rankine cycle power plant with wet cooling towers that produced the samelevel of electric generation. Dry cooling towers can be used to significantly reduce plant water consumption; however,this can result in up to a 10% reduction in power plant efficiency. Waste water discharge from the plant is also anissue. Blowdown from the steam cycle, demineralizer, and cooling towers must typically be sent to a evaporation ponddue to the high mineral content or due to chemicals that have been added to the water. Water requirements are shownin Section 5.

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Land: Parabolic trough plants require a significant amount of land that typically cannot be used concurrently for otheruses. Parabolic troughs require the land to be graded level. One opportunity to minimize the development ofundisturbed lands is to use parcels of marginal and fallow agricultural land instead. A study sponsored by theCalifornia Energy Commission determined that 27,000 MW of STE plants could be built on marginal and fallowe

agricultural land in Southern California [12]. A study for the state of Texas showed that land use requirements forparabolic trough plants are less that those of most other renewable technologies (wind, biomass, hydro) and also lessthan those of fossil when mining and drilling requirements are included [13]. Current trough technology producesabout 100 kWh/yr/m of land. 2

Hybrid Operation: Solar/fossil hybrid plant designs will operate with fossil fuels during some periods. During thesetimes, the plant will generate emissions consistent with the fuel.

3.0 Technology Assumptions and Issues

Trough Technology: The experience from the nine SEGS plants demonstrates the commercial nature of parabolictrough solar collector and power plant technologies. Given this experience, it is assumed that future parabolic troughplant designs will continue to focus on the Luz parabolic trough collector technology and Rankine cycle steam powerplants. The next plants built are assumed to copy the 80 MW SEGS plant design and use the third generation LuzSystem Three parabolic trough collector.

Cost and Performance Data: The information presented is based on existing SEGS plant designs and operationalexperience. In addition, much of the cost data comes from PilkSolar [1] who has been actively pursuing opportunitiesfor parabolic trough developments in many international locations. Performance projections assume a solar resourcethat would be typical for plants located in the California Mojave Desert. PilkSolar developed a detailed hour-by-hoursimulation code to calculate the expected annual performance of parabolic trough plants. This model has beenvalidated by baselining it against an operating SEGS plant. The model was found to reproduce real plant performancewithin 5% on an annual basis. The model can be used to perform design trade-off studies with a reasonable level ofconfidence.

Power Plant Size: Increasing plant size is one of the easiest ways to reduce the cost of solar electricity from parabolictrough power plants. Studies have shown that doubling the size reduces the capital cost by approximately 12-14% [1].Figure 5 shows an example of how the levelized energy cost for solar electricity decreases by over 60% by onlyincreasing the plant size. Cost reduction typically comes from three areas. First, the increased manufacturing volumeof collectors for larger plants drives the cost per square meter down. Second, a power plant that is twice the size willnot cost twice as much to build. Third, the O&M costs for larger plants will typically be less on a per kilowatt basis.For example, it takes about the same number of operators to operate a 10 MW plant as it does a 400 MW plant [2].Power plant maintenance costs will be reduced with larger plants but solar field maintenance costs will scale morelinearly with solar field size.

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Figure 5. Effect of power plant size on normalized levelized COE.

The latest parabolic trough plants built were 80 MW in size. This size was a result of limitations imposed by theFederal government. Luz had investigated sizes up to 160 MW. The main concern with larger plants is the increasedsize of the solar field which impacts HTF pumping parasitics. In future plants, pumping parasitics will be reduced byreplacing the flexible hoses with the new ball joint assemblies [8], allowing for plants in excess of the 160 MW sizeto be built.

Hybridization: Hybridization with a fossil fuel offers a number of potential benefits to solar plants including: reducedrisk to investors, improved solar-to-electric conversion efficiency, and reduced levelized cost of energy from the plant[14]. Furthermore, it allows the plant to provide firm, dispatchable power.

Since fossil fuel is currently cheap, hybridization of a parabolic trough plant is assumed to provide a good opportunityto reduce the average cost of electricity from the plant. Hybridizing parabolic trough plants has been accomplishedin a number of ways. All of the existing SEGS plants are hybrid solar/fossil designs that are allowed to take up to 25%of their annual energy input to the plant from fossil fuel. Fossil energy can be used to superheat solar generated steam(SEGS I), fossil energy can be used in a separate fossil-fired boiler to generate steam when insufficient solar energyis available (SEGS II-VII), or fossil energy can be used in an oil heater in parallel with the solar field when insufficientsolar energy is available (SEGS VIII-IX). The decision on type of hybridization has been primarily an economicdecision. However, it is clear from the SEGS experience that hybridization of the plants has been essential to theoperational success of the projects. The alternative ISCCS design offers a number of potential advantages to both the solar plant and the combined cycleplant. The solar plant benefits because the incremental cost of increasing the size of the steam turbine in the combinedcycle is significantly less than building a complete stand-alone power plant. O&M costs are reduced because the costof operation and maintenance on the conventional portion of the plant is covered by the combined cycle costs. Also,the net annual solar-to-electric efficiency is improved because solar input is not lost waiting for the turbine plant to startup, and because the average turbine efficiency will be higher since the turbine will always be running at 50% load orabove. The combined cycle benefits because the fossil conversion efficiency is increased during solar operation since

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Figure 6. Effect of hybridization on LEC.

the gas turbine waste heat can be used more efficiently. Solar output will also help to offset the normal reduction inperformance experienced by combined cycle plants during hot periods. Figure 6 shows how the LEC for an 80 MWsolar increment ISCCS plant compares to those of a solar only SEGS and a conventional hybrid SEGS plant.

Thermal Storage: The availability of efficient and low-cost thermal storage is important for the long-term cost reductionof trough technology and significantly increases potential market opportunities. A parabolic trough plant with no fossilbackup or thermal storage, located in the Mojave Desert, should be capable of producing electricity up to about a 25%annual capacity factor. The addition of thermal storage could allow the plant to dispatch power to non-solar times ofthe day and could allow the solar field to be oversized to increase the plant’s annual capacity factor to about 50%.Attempting to increase the annual capacity factor much above 50% would result in significant dumping of solar energyduring summer months. An efficient 2-tank HTF thermal storage system has been demonstrated at the SEGS I plant.However, it operates at a relatively low solar field HTF outlet temperature (307ºC/585ºF), and no cost effective thermalstorage system has yet been developed for the later plants that operate at higher HTF temperatures (390ºC/734ºF) andrequire a more stable (and expensive) HTF. A study of applicable thermal storage concepts for parabolic trough plantshas recommended a concrete and steel configuration, though other methods are possible [6].

Advanced Trough Collector: One of the main performance improvements possible for single axis tracking parabolictrough collectors is to tilt the axis of rotation above horizontal. Luz looked at tilting their LS-4 design 8º abovehorizontal and estimated a 9% increase in annual solar field performance.

Direct Steam Generation (DSG): In the DSG concept, steam is generated directly in the parabolic trough collectors.This saves cost by eliminating the need for the HTF system and reduces the efficiency loss of having to use a heatexchanger to generate steam. The solar field operating efficiency should improve due to lower average operatingtemperatures and improved heat transfer in the collector. The trough collectors require some modification due to thehigher operating pressure and lower fluid flow rates. Control of a DSG solar field will likely be more complicated thanthe HTF systems and may require a more complex design layout and a tilted collector. DSG offers a number of

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advantages over current HTF systems, but controllability and O&M risks have yet to be resolved. A pilotdemonstration of DSG technology is in progress at the Plataforma Solar de Almería in Spain [15].

Project Development Issues: The environment in which a trough project is developed will have a significant impacton the eventual cost of the technology. As mentioned in the Overview of Solar Thermal Technologies, buildingmultiple plants in a solar power park environment, the type of project financing, and access to incentives which levelizethe tax burden between renewables and conventional power technologies can dramatically improve the economics ofSTE technologies. Although project financing and tax equity issues are not addressed in this doccument, thetechnology cases presented in Section 4 assume that multiple projects are built at the same site in a solar power parkenvironment. This assumption seems reasonable since a stand-alone plant would be significantly more expensive andless likely to be built.

Performance Adjustment Factor for Solar Radiation at Different Sites: Direct normal insolation (DNI) resources varywidely by location. The performance projections presented in the following sections assume a solar resource equivalentto Barstow, California. Table 3 shows the DNI resources for other locations [2,16] and the approximate change inperformance that might be expected due to the different solar radiation resources. From Table 3 it can be seen that a1% change in DNI results in a greater than 1% change in electric output. It is important to note that the table does notcorrect for latitude which can have a significant impact on solar performance. In general, solar field size can beincreased to offset reduced performance resulting from lower clear sky radiation levels, but increased size cannot helpreductions resulting from increased cloud cover, unless the plant also includes thermal storage.

4.0 Performance and Cost

Table 4 summarizes the performance and cost indicators for the parabolic trough system characterized in this report.

4.1 Evolution Overview

The parabolic trough plant technology discussion presented focuses on the development of Luz parabolic troughcollector designs and the continued use of Rankine cycle steam power plants. Although the ISCCS concept is likelyto be used for initial reintroduction of parabolic trough plants and could continue to be a popular design alternative forsome time into the future, the approach used here is to look at how parabolic trough plants will need to develop if theyare going to be able to compete with conventional power technologies and provide a significant contribution to theworld’s energy mix in the future. To achieve these long-term objectives, trough plants will need to continue to movetowards larger solar only Rankine cycle plants and develop efficient and cost effective thermal storage to increaseannual capacity factors.

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Table 3. Solar radiation performance adjustment.

LocationSite Annual Relative Relative

Latitude DNI Solar Solar Electric(kWh/m )2 Resource Output

United States

Barstow, California 35ºN 2,725 1.00 1.00

Las Vegas, Nevada 36ºN 2,573 0.94 0.93

Tucson, Arizona 32ºN 2,562 0.94 0.92

Alamosa, Colorado 37ºN 2,491 0.91 0.89

Albuquerque, New Mexico 35ºN 2,443 0.90 0.87

El Paso, Texas 32ºN 2,443 0.90 0.87

International

Northern Mexico 26-30ºN 2,835 1.04 1.05

Wadi Rum, Jordan 30ºN 2,500 0.92 0.89

Ouarzazate, Morocco 31ºN 2,364 0.87 0.83

Crete 35ºN 2,293 0.84 0.79

Jodhpur, India 26ºN 2,200 0.81 0.75

1997 Technology: The 1997 baseline technology is assumed to be the 30 MW SEGS VI plant [17]. The SEGS VI plantis a hybrid solar/fossil plant that uses 25% fossil input to the plant on an annual basis in a natural gas-fired steam boiler.The plant uses the second generation Luz LS-2 parabolic trough collector technology. The solar field is composed of800 LS-2 SCAs (188,000 m of mirror aperture) arranged in 50 parallel flow loops with 16 SCAs per loop. Similar2

to the 80 MW plants, the power block uses a reheat steam turbine and the solar field operates at the same HTF outlettemperature of 390ºC (734ºF). Solar steam is generated at 10 MPa and 371ºC (700ºF). The plant is hybridized witha natural gas fired steam boiler which generates high pressure steam at 10 MPa and 510ºC (950ºF).

2000 Technology: The year 2000 plant is assumed to be the next parabolic trough plant built which is assumed to bethe 80 MW SEGS X design [4]. The primary changes from the 1997 baseline technology is that this plant sizeincreases to 80 MW, the LS-3 collector is used in place of the LS-2, the HCE uses an improved selective coating, andflex hoses have been replaced with ball joint assemblies. The solar field is composed of 888 LS-3 SCAs (510,120 m2

of mirror aperture) arranged in 148 parallel flow loops with 6 SCAs per loop. The plant is hybridized with a naturalgas fired HTF heater.

2005 Technology: The power plant is scaled up to 160 MW. Six hours of thermal storage is added to the plant to allowthe plant to operate at up to a 40% annual capacity factor from solar input alone. No backup fossil operating capabilityis included. The LS-3 parabolic trough collector continues to be used, but the solar field size is scaled up to allow theplant to achieve higher annual capacity factor using 2,736 SCAs (1,491,120 m of mirror aperture) arranged in 4562

parallel flow loops with 6 SCAs per loop.

2010 Technology: The power plant is scaled up to 320 MW and operates to an annual capacity factor of 50% from solarinput. Again no fossil backup operation is included. This design incorporated the next generation of trough

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Table 4. Performance and cost indicators.

INDICATORNAME

1997 2000 2005 2010 2020 2030SEGS VI SEGS LS-3 SEGS LS-3 SEGS LS-4 SEGS DSG SEGS DSG *

Base Case 25% Fossil w/Storage w/Storage w/Storage w/Storage †

UNITS +/-% +/-% +/-% +/-% +/-% +/-%Plant Design

Plant Size MW 30 80 161 320 320 320Collector Type LS-2 LS-3 LS-3 LS-4 LS-4 LS-4Solar Field Area m 188,000 510,120 1,491,120 3,531,600 3,374,640 3,204,6002

Thermal Storage Hours 0 0 6 10 10 10MWh 0 0 3,000 10,042 9,678 9,678t

Performance

Capacity Factor % 34 34 40 50 50 50Solar Fraction (Net Elec.) % 66 75 100 100 100 100Direct Normal Insolation kWh/m -yr 2,891 2,725 2,725 2,725 2,725 2,7252

Annual Solar to Elec. Eff. % 10.7 12.9 13.8 14.6 15.3 16.1Natural Gas (HHV) GJ 350,000 785,000 0 0 0 0Annual Energy Production GWh/yr 89.4 238.3 564.1 1,401.6 1,401.6 1,401.6Development AssumptionsPlants Built Per Year 2 2 2 3 3 3Plants at a Single Site 5 5 5 5 5 5Competitive Bidding Adj. 1.0 1.0 0.9 0.9 0.9 0.9O&M Cost Adjustment 1.0 0.9 0.85 0.7 0.6 0.6

Operations and Maintenance Cost

Labor $/kW-yr 32 25 21 25 14 25 11 25 11 25Materials 31 25 31 25 29 25 23 25 23 25Total O&M Costs 107 63 52 43 34 34Notes:1. The columns for "+/- %" refer to the uncertainty associated with a given estimate.2. The construction period is assumed to be 1 year.3. Totals may be slightly off due to rounding.

SEGS VI Capital cost of $99.3M in 1989$ is adjusted to $119.2M in 1997$. Limited breakdown of costs by subsystem is available. Performance and O&M costs based on actual*

data.By comparison, an ISCCS plant built in 2000 with an 80 MW solar increment would have a solar capital cost of $2,400/kW, annual O&M cost of $48/kW, and an annual net solar-to-†

electric efficiency of 13.5%[1].To convert to peak values, the effect of thermal storage must be removed. A first-order estimate can be obtained by dividing installed costs by the solar multiple (i.e., SM={peak‡

collected solar thermal power}÷ {power block thermal power}).

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Table 4. Performance and cost indicators.(cont.)

INDICATORNAME

1997 2000 2005 2010 2020 2030SEGS VI SEGS LS-3 SEGS LS-3 SEGS LS-4 SEGS DSG SEGS DSG *

Base Case 25% Fossil w/Storage w/Storage w/Storage w/Storage †

UNITS +/-% +/-% +/-% +/-% +/-% +/-%Capital CostStructures/Improvements $/kW 54 79 15 66 15 62 15 60 15 58 15Collector System 3,048 1,138 25 1,293 25 1,327 25 1,275 25 1,158 25Thermal Storage System 0 0 392 +50/-25 528 +50/-25 508 +50/-25 508 +50/-25Steam Gen or HX System 109 15 90 15 81 15 80 15 79 15Aux Heater/Boiler 120 164 15 0 15 0 15 0 15 0 15Electric Power Generation 476 15 347 15 282 15 282 15 282 15Balance of Plant 750 202 15 147 15 120 15 120 15 120 15Subtotal (A) 3,972 2,168 2,336 2,400 2,326 2,205Engr, Proj./Const. Manag. A * 0.08 174 187 192 186 176Subtotal (B) 3,972 2,342 2,523 2,592 2,512 2,382Project/Process Conting B * 0.15 351 378 389 377 357Total Plant Cost 3,972 2,693 2,901 2,981 2,889 2,739Land @ $4,942/ha 11 15 18 17 17Total Capital Requirements $/kW 3,972 2,704 2,916 2,999 2,907 2,756

$/kW 3,972 2,704 1,700 1,400 1,350 1,300peak‡

$/m 634 424 315 272 276 2752

Operations and Maintenance Cost

Labor $/kW-yr 32 25 21 25 14 25 11 25 11 25Materials 31 25 31 25 29 25 23 25 23 25Total O&M Costs 107 63 52 43 34 34Notes:1. The columns for "+/- %" refer to the uncertainty associated with a given estimate.2. The construction period is assumed to be 1 year.3. Totals may be slightly off due to rounding.

SEGS VI Capital cost of $99.3M in 1989$ is adjusted to $119.2M in 1997$. Limited breakdown of costs by subsystem is available. Performance and O&M costs based on actual*

data.By comparison, an ISCCS plant built in 2000 with an 80 MW solar increment would have a solar capital cost of $2,400/kW, annual O&M cost of $48/kW, and an annual net solar-to-†

electric efficiency of 13.5%[1].To convert to peak values, the effect of thermal storage must be removed. A first-order estimate can be obtained by dividing installed costs by the solar multiple (i.e., SM={peak‡

collected solar thermal power}÷ {power block thermal power}).

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collector, possibly something like the Luz LS-4 advanced trough collector (over 3,500,000 m of mirror aperture). The2

solar field continues to use a heat transfer fluid but the collector is assumed to have a fixed tilt of 8º.

2020 - 2030 Technology: Power plant size is assumed to remain at 320 MW with 50% annual capacity factor. Thisdesign assumes the technology will incorporate direct steam generation (DSG) into the collector in the solar field (over3,200,000 m of mirror aperture).2

4.2 Performance and Cost Discussion

Plant Performance

Increasing the performance of the solar collectors and power plant are one of the primary opportunities for reducingthe cost of trough technology. Collector performance improvements can come from developing new more efficientcollector technologies and components but often also by improving the reliability and lifetime of existing components.Table 4 shows the annual performance and net solar-to-electric efficiency of each of the technology cases describedabove.

The 1997 baseline case performance represents the actual 1996 performance of the 30 MW SEGS VI plant (its 8th yearof operation). During 1996, the SEGS VI plant had an annual net solar-to-electric efficiency of 10.7% [10,18]. Thisperformance was somewhat reduced by the high level of HCE breakage at the plant (5% with broken glass and 1% withlost vacuum). Since the HCE problems at SEGS VI are due to a design error that was later corrected, we assume thatHCE breakage at future plants should remain below 1%, a number consistent with the experience at the SEGS V plant.The SEGS VI plant was selected as the baseline system because substantially more cost and performance data isavailable and more analysis of plant performance has been completed than at either of the existing 80 MW SEGSplants. Note, even though only 25% of the annual energy input to the plant comes from natural gas, since this energyis converted only at the highest turbine cycle efficiency, 34% of the annual electric output from the plant comes fromgas energy.

The year 2000 technology shows a 20% improvement in net solar to electric efficiency over the 1997 baseline systemperformance. This is achieved by using current technologies and designs, by reducing HCE heat losses and electricparasitics. New HCEs have an improved selective surface with a higher absorptance and a 50% lower emittance. Thishelps reduce trough receiver heat losses by one third. The ball joint assemblies and the reduced number of SCAs percollector loop (6 for LS-3 versus 16 for LS-2 collectors) will reduce HTF pumping parasitics. Adjusting for reducedparasitics, improved HCE selective surface, and lower HCE breakage, a new 80 MW plant would be expected to havea net solar-to-electric efficiency of 12.9%.

The 2005 technology shows a 7% increase in efficiency primarily as a result of adding thermal storage. Thermalstorage eliminates dumping of solar energy during power plant start-up and during peak solar conditions when solarfield thermal delivery is greater than power plant capacity. Thermal storage also allows the power plant to operateindependently of the solar field. This allows the power plant to operate near full load efficiency more often, improvingthe annual average power block efficiency. The thermal storage system is assumed to have an 85% round-tripefficiency. Minor performance improvements also result from scaling the plant up to 160 MW from 80 MW. Annualnet solar-to-electric efficiency increases to 13.8% [1].

The 2010 technology shows a 6% increase in net solar-to-electric efficiency primarily due to the use of the tiltedcollector. Power plant efficiency improves slightly due to larger size of the 320 MW power plant. Thermal storagehas been increased to 10 hours and the solar field size increased to allow the plant to operate up to a 50% annual

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capacity factor. As a result, more solar energy must be stored before it can be used to generate electricity, thus the 85%round-trip efficiency of the thermal storage system tends to have a larger impact on annual plant performance. Theresulting annual net solar-to-electric efficiency increases to 14.6%.

The 2020 and 2030 technologies show 5% and 10% improvements in performance over the 2010 trough technology.The is due to the introduction of the direct steam generation trough collector technology. DSG improves the efficiencyin the solar field and reduces equipment costs by eliminating the HTF system. Power cycle efficiency is assumed toimprove due to higher solar steam temperatures. Solar parasitics are reduced through elimination of HTF pumps.Although feedwater must still be pumped through the solar field, it is pumped at a much lower mass flow rate. Thisdesign also assumes that a low cost thermal storage system with an 85% round-trip efficiency is developed for use withthe DSG solar field. Conversion to the DSG collector system could allow the net solar-to-electric efficiency to increaseto over 16% by 2030. The changes between 2020 and 2030 are assumed to be evolutionary improvements and finetuning of the DSG technology.

Cost Reductions

Table 4 shows the total plant capital cost for each technology case on a $/kW/m basis. The technology shows a 30%2

cost reduction on a $/kW basis and a 55% reduction on a $/m basis. These cost reductions are due to: larger plants2

being built, increased collector production volumes, building projects in solar power park developments, and savingsthrough competitive bidding. In general, the per kW capital cost of power plants decreases as the size of the plantincreases. For trough plants, a 49% reduction in the power block equipment cost results by increasing the power plantsize from 30 to 320 MW. The increased production volume of trough solar collectors, as a result of larger solar fieldsand multiple plants being built in the same year, reduces trough collector costs by 44%. Power parks allow forefficiencies in construction and cost reduction through competitive bidding of multiple projects. A 10% cost reductionis assumed for competitive bidding in later projects.

The annual operation and maintenance (O&M) costs for each technology are shown in Table 4. O&M costs show areduction of almost 80%. This large cost reduction is achieved through increasing size of the power plant, increasingthe annual solar capacity factor, operating plants in a solar power park environment, and continued improvements inO&M efficiencies. Larger plants reduce operator labor costs because approximately the same number of people arerequired to operate a 320 MW plant as are required for a 30 MW plant. The solar power park assumes that five plantsare co-located and operated by the same company resulting in a 25% O&M savings through reduced overhead andimproved labor and material efficiencies. In addition, about one third of the cost reduction is assumed to occur becauseof improved O&M efficiency resulting from improved plant design and O&M practices based on the results of the KJCO&M Cost Reduction Study [8].

Summary

The technology cases presented above show that a significant increase in performance and reduction in cost is possiblefor parabolic trough solar thermal electric technologies as compared with the 1997 baseline technology case. Figure7 shows the relative impacts of the various cost reduction opportunities or performance improvements on the baselinesystem's levelized cost of energy. It is significant to note that the majority of the cost reduction opportunities do notrequire any significant technology development. Conversely, significant progress must be made in these non-technology areas if parabolic troughs are to be competitive with conventional power technologies and make anysignificant market penetration.

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Figure 7. Cost reduction opportunities for parabolic trough plants.

5.0 Land, Water, and Critical Materials Requirements

Land and water requirements are shown in the table below for each of the technology cases. The land and waterrequirements initially increase as a result of increasing plant annual operating capacity factors. The land requirementsbegin to decrease as a result of improving solar-to-electric efficiencies. Note, the plant capacity factor increases overtime because future plants are assumed to include thermal storage and proportionally larger solar fields.

Table 4. Resource requirements [2].

IndicatorName Units 1997 2000 2005 2010 2020 2030

Base Year

Plant Size MW 30 80 161 320 320 320

Land ha/MW 2.2 2.2 3.1 3.7 3.6 3.4

ha 66 176 500 1,190 1,150 1,090

Water m /MW-yr 18,500 14,900 17,500 21,900 21,900 21,9003

6.0 References

1. Status Report on Solar Thermal Power Plants, Pilkington Solar International: 1996. Report ISBN 3-9804901-0-6.

2. Assessment of Solar Thermal Trough Power Plant Technology and Its Transferability to the Mediterranean Region- Final Report, Flachglas Solartechnik GMBH, for European Commission Directorate General I ExternalEconomic Relations, and Centre de Developpement des Energies Renouvelables and Grupo Endesa, Cologne,Germany: June 1994.

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3. Integrated Solar Combined Cycle Systems (ISCCS) Using Parabolic Trough Technology, Phase 1B Technicaland Financial Review, Spencer Management Associates, Diablo, CA: March 1996, draft.

4. "Solar Electric Generating System IX Technical Description", LUZ International Limited: 1990.

5. Lotker, M., Barriers to Commercialization of Large-Scale Solar Electricity: Lessons Learned from the LUZExperience, Sandia National Laboratories, Albuquerque, New Mexico: 1991. Report SAND91-7014.

6. Winter, C.-J., R. Sizmann, and L. Vant-Hull, eds., Solar Power Plants - Fundamentals, Technology, Systems,Economics. Springer-Verlag, Berlin, 1990, ISBN 3-540-18897-5.

7. O&M Cost Reduction in Solar Thermal Electric Power Plants - Interim Report on Project Status, KJC OperatingCompany, for Sandia National Laboratories: September 1, 1994.

8. O&M Cost Reduction in Solar Thermal Electric Power Plants - 2nd Interim Report on Project Status, KJCOperating Company, for Sandia National Laboratories: July 1, 1996.

9. Dudley, V., G. Kolb, A. R. Mahoney, T. Mancini, C. Matthews, M. Sloan, and D. Kearney, Test Results: SEGSLS-2 Solar Collector, Sandia National Laboratories, Albuquerque, New Mexico: December 1994. ReportSAND94-1884.

10. Cohen, G., and S. Frier, “Ten Years of Solar Power Plant Operation in the Mojave Desert”, Proceedings of Solar97, the 1997 ASES Annual Conference, Washington, D.C. (April, 1997).

11. Fugitive Emissions Testing - Final Report, AeroVironment, Inc., for KJC Operating Company, Monrovia, CA:January 1995.

12. Technical Potential of Alternative Technologies - Final Report, Regional Economic Research, Inc., for CaliforniaEnergy Commission, Contract No. 500-89-001, San Diego, CA: December 2, 1991.

13. Texas Renewable Energy Resource Assessment: Survey, Overview & Recommendations, Virtus Energy ResearchAssociates, for the Texas Sustainable Energy Development Council, July, 1995, ISBN 0-9645526-0-4.

14. Williams, T., M. Bohn, and H. Price, “Solar Thermal Electric Hybridization Issues”, Proceedings of theASME/JSME/JSES International Solar Energy Conference, Maui, HI (March 19-24, 1995).

15. Muller, M., Direct Solar Steam in Parabolic Trough Collectors (DISS), Plataforma Solar de Almeria (PSA),CIEMAT and DLR, May, 1994, ISBN 84-605-1479-X.

16. Marion, W., and S. Wilcox, Solar Radiation Data Manual for Flat-Plate and Concentrating Collectors, NationalRenewable Energy Laboratory, Golden, Colorado: April 1994. Report NREL/TP-463-5607.

17. Kearney, D., and C. Miller, Solar Electric Generating System VI - Technical Evaluation of Project Feasibility,LUZ Partnership Management, Inc.: January 15, 1988.

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18. Kolb, G. J., “Evaluation of Power Production from the Solar Electric Generating Systems at Kramer Junction:1988 to 1993”, Solar Engineering - 1995, Proceedings of the ASME Solar Energy Conference, Maui, HI (March19-24, 1995).